Jump to
S1C2
Energy calculated at B3LYP/STO-3G
| hartrees |
Energy at 0K | -214.241647 |
Energy at 298.15K | |
HF Energy | -214.241647 |
Nuclear repulsion energy | 114.320157 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3LYP/STO-3G
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A' |
3544 |
3163 |
0.20 |
32.51 |
0.69 |
0.82 |
2 |
A' |
3440 |
3070 |
1.58 |
56.85 |
0.28 |
0.43 |
3 |
A' |
3389 |
3025 |
15.20 |
27.33 |
0.15 |
0.25 |
4 |
A' |
3194 |
2851 |
12.98 |
64.80 |
0.12 |
0.21 |
5 |
A' |
1851 |
1652 |
1.39 |
5.77 |
0.08 |
0.15 |
6 |
A' |
1652 |
1474 |
0.89 |
19.22 |
0.71 |
0.83 |
7 |
A' |
1545 |
1379 |
1.17 |
10.81 |
0.57 |
0.73 |
8 |
A' |
1494 |
1334 |
21.04 |
9.23 |
0.58 |
0.73 |
9 |
A' |
1391 |
1241 |
1.56 |
16.96 |
0.56 |
0.72 |
10 |
A' |
1225 |
1093 |
10.00 |
2.27 |
0.75 |
0.85 |
11 |
A' |
1078 |
962 |
6.11 |
5.00 |
0.73 |
0.85 |
12 |
A' |
935 |
834 |
1.78 |
5.01 |
0.23 |
0.37 |
13 |
A' |
604 |
539 |
0.71 |
1.65 |
0.75 |
0.85 |
14 |
A' |
227 |
203 |
0.51 |
0.86 |
0.52 |
0.68 |
15 |
A" |
3278 |
2925 |
12.21 |
50.69 |
0.75 |
0.86 |
16 |
A" |
1313 |
1171 |
1.00 |
9.06 |
0.75 |
0.86 |
17 |
A" |
1103 |
984 |
8.68 |
0.15 |
0.75 |
0.86 |
18 |
A" |
1083 |
966 |
0.70 |
0.48 |
0.75 |
0.86 |
19 |
A" |
1001 |
893 |
19.65 |
0.11 |
0.75 |
0.86 |
20 |
A" |
577 |
515 |
5.31 |
6.25 |
0.75 |
0.86 |
21 |
A" |
136 |
121 |
0.74 |
2.81 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17029.7 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 15197.3 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3LYP/STO-3G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
-0.984 |
0.000 |
C2 |
-0.964 |
0.233 |
0.000 |
C3 |
-0.536 |
1.496 |
0.000 |
F4 |
1.351 |
-0.588 |
0.000 |
H5 |
-1.224 |
2.350 |
0.000 |
H6 |
0.538 |
1.723 |
0.000 |
H7 |
-2.035 |
-0.016 |
0.000 |
H8 |
-0.220 |
-1.618 |
0.898 |
H9 |
-0.220 |
-1.618 |
-0.898 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5521 | 2.5376 | 1.4079 | 3.5513 | 2.7600 | 2.2537 | 1.1214 | 1.1214 |
C2 | 1.5521 | | 1.3342 | 2.4562 | 2.1331 | 2.1156 | 1.1002 | 2.1878 | 2.1878 | C3 | 2.5376 | 1.3342 | | 2.8120 | 1.0960 | 1.0974 | 2.1299 | 3.2570 | 3.2570 | F4 | 1.4079 | 2.4562 | 2.8120 | | 3.9067 | 2.4503 | 3.4346 | 2.0822 | 2.0822 | H5 | 3.5513 | 2.1331 | 1.0960 | 3.9067 | | 1.8696 | 2.5016 | 4.1906 | 4.1906 | H6 | 2.7600 | 2.1156 | 1.0974 | 2.4503 | 1.8696 | | 3.1059 | 3.5419 | 3.5419 | H7 | 2.2537 | 1.1002 | 2.1299 | 3.4346 | 2.5016 | 3.1059 | | 2.5826 | 2.5826 | H8 | 1.1214 | 2.1878 | 3.2570 | 2.0822 | 4.1906 | 3.5419 | 2.5826 | | 1.7967 | H9 | 1.1214 | 2.1878 | 3.2570 | 2.0822 | 4.1906 | 3.5419 | 2.5826 | 1.7967 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
122.915 |
|
C1 |
C2 |
H7 |
115.306 |
C2 |
C1 |
F4 |
112.062 |
|
C2 |
C1 |
H8 |
108.763 |
C2 |
C1 |
H9 |
108.763 |
|
C2 |
C3 |
H5 |
122.444 |
C2 |
C3 |
H6 |
120.621 |
|
C3 |
C2 |
H7 |
121.780 |
F4 |
C1 |
H8 |
110.303 |
|
F4 |
C1 |
H9 |
110.303 |
H5 |
C3 |
H6 |
116.934 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.034 |
|
|
|
2 |
C |
-0.084 |
|
|
|
3 |
C |
-0.164 |
|
|
|
4 |
F |
-0.100 |
|
|
|
5 |
H |
0.078 |
|
|
|
6 |
H |
0.081 |
|
|
|
7 |
H |
0.076 |
|
|
|
8 |
H |
0.073 |
|
|
|
9 |
H |
0.073 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.840 |
-0.376 |
0.000 |
0.920 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.170 |
0.656 |
0.000 |
y |
0.656 |
-20.529 |
0.000 |
z |
0.000 |
0.000 |
-22.558 |
|
Traceless |
| x | y | z |
x |
-0.627 |
0.656 |
0.000 |
y |
0.656 |
1.835 |
0.000 |
z |
0.000 |
0.000 |
-1.208 |
|
Polar |
3z2-r2 | -2.416 |
x2-y2 | -1.641 |
xy | 0.656 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.751 |
0.195 |
0.000 |
y |
0.195 |
3.941 |
0.000 |
z |
0.000 |
0.000 |
1.244 |
<r2> (average value of r
2) Å
2
<r2> |
81.368 |
(<r2>)1/2 |
9.020 |
Jump to
S1C1
Energy calculated at B3LYP/STO-3G
| hartrees |
Energy at 0K | -214.241079 |
Energy at 298.15K | |
HF Energy | -214.241079 |
Nuclear repulsion energy | 111.938866 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3LYP/STO-3G
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A |
3538 |
3157 |
0.04 |
35.06 |
0.71 |
0.83 |
2 |
A |
3441 |
3071 |
2.12 |
51.01 |
0.27 |
0.43 |
3 |
A |
3387 |
3023 |
13.35 |
31.22 |
0.14 |
0.24 |
4 |
A |
3309 |
2953 |
10.86 |
34.17 |
0.75 |
0.86 |
5 |
A |
3208 |
2862 |
14.29 |
49.13 |
0.15 |
0.27 |
6 |
A |
1844 |
1646 |
0.18 |
7.49 |
0.10 |
0.18 |
7 |
A |
1647 |
1470 |
0.33 |
13.18 |
0.75 |
0.86 |
8 |
A |
1573 |
1404 |
4.90 |
12.23 |
0.47 |
0.64 |
9 |
A |
1480 |
1321 |
19.85 |
6.30 |
0.72 |
0.84 |
10 |
A |
1399 |
1249 |
3.13 |
15.26 |
0.57 |
0.72 |
11 |
A |
1327 |
1184 |
3.65 |
15.50 |
0.74 |
0.85 |
12 |
A |
1214 |
1084 |
0.76 |
2.76 |
0.59 |
0.74 |
13 |
A |
1181 |
1054 |
16.74 |
4.01 |
0.54 |
0.70 |
14 |
A |
1104 |
985 |
9.17 |
0.43 |
0.73 |
0.84 |
15 |
A |
1014 |
905 |
3.48 |
0.43 |
0.48 |
0.65 |
16 |
A |
1006 |
898 |
15.56 |
0.29 |
0.38 |
0.55 |
17 |
A |
964 |
860 |
5.26 |
2.88 |
0.21 |
0.35 |
18 |
A |
678 |
605 |
4.59 |
4.27 |
0.59 |
0.74 |
19 |
A |
421 |
376 |
0.33 |
2.23 |
0.50 |
0.67 |
20 |
A |
332 |
296 |
2.23 |
3.30 |
0.75 |
0.86 |
21 |
A |
89 |
79 |
0.21 |
3.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 17079.2 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 15241.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3LYP/STO-3G
Point Group is C1
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
-0.639 |
0.415 |
0.350 |
C2 |
0.685 |
-0.384 |
0.272 |
C3 |
1.819 |
0.104 |
-0.240 |
F4 |
-1.672 |
-0.221 |
-0.379 |
H5 |
2.742 |
-0.488 |
-0.279 |
H6 |
1.881 |
1.125 |
-0.638 |
H7 |
0.643 |
-1.412 |
0.663 |
H8 |
-0.946 |
0.512 |
1.423 |
H9 |
-0.466 |
1.447 |
-0.044 |
Atom - Atom Distances (Å)
|
C1 |
C2 |
C3 |
F4 |
H5 |
H6 |
H7 |
H8 |
H9 |
C1 | | 1.5491 | 2.5468 | 1.4151 | 3.5556 | 2.7982 | 2.2540 | 1.1208 | 1.1177 |
C2 | 1.5491 | | 1.3361 | 2.4505 | 2.1316 | 2.1295 | 1.1003 | 2.1887 | 2.1860 | C3 | 2.5468 | 1.3361 | | 3.5082 | 1.0970 | 1.0975 | 2.1203 | 3.2522 | 2.6574 | F4 | 1.4151 | 2.4505 | 3.5082 | | 4.4225 | 3.8079 | 2.8033 | 2.0771 | 2.0856 | H5 | 3.5556 | 2.1316 | 1.0970 | 4.4225 | | 1.8627 | 2.4794 | 4.1830 | 3.7533 | H6 | 2.7982 | 2.1295 | 1.0975 | 3.8079 | 1.8627 | | 3.1081 | 3.5517 | 2.4422 | H7 | 2.2540 | 1.1003 | 2.1203 | 2.8033 | 2.4794 | 3.1081 | | 2.6087 | 3.1468 | H8 | 1.1208 | 2.1887 | 3.2522 | 2.0771 | 4.1830 | 3.5517 | 2.6087 | | 1.8047 | H9 | 1.1177 | 2.1860 | 2.6574 | 2.0856 | 3.7533 | 2.4422 | 3.1468 | 1.8047 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
C2 |
C3 |
123.779 |
|
C1 |
C2 |
H7 |
115.548 |
C2 |
C1 |
F4 |
111.440 |
|
C2 |
C1 |
H8 |
109.071 |
C2 |
C1 |
H9 |
109.038 |
|
C2 |
C3 |
H5 |
122.041 |
C2 |
C3 |
H6 |
121.792 |
|
C3 |
C2 |
H7 |
120.670 |
F4 |
C1 |
H8 |
109.436 |
|
F4 |
C1 |
H9 |
110.314 |
H5 |
C3 |
H6 |
116.165 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
-0.037 |
|
|
|
2 |
C |
-0.083 |
|
|
|
3 |
C |
-0.157 |
|
|
|
4 |
F |
-0.100 |
|
|
|
5 |
H |
0.080 |
|
|
|
6 |
H |
0.076 |
|
|
|
7 |
H |
0.078 |
|
|
|
8 |
H |
0.072 |
|
|
|
9 |
H |
0.072 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.652 |
0.384 |
0.488 |
0.900 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-22.693 |
-0.547 |
-1.043 |
y |
-0.547 |
-20.941 |
-0.571 |
z |
-1.043 |
-0.571 |
-22.285 |
|
Traceless |
| x | y | z |
x |
-1.080 |
-0.547 |
-1.043 |
y |
-0.547 |
1.547 |
-0.571 |
z |
-1.043 |
-0.571 |
-0.467 |
|
Polar |
3z2-r2 | -0.934 |
x2-y2 | -1.752 |
xy | -0.547 |
xz | -1.043 |
yz | -0.571 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.905 |
0.239 |
-0.615 |
y |
0.239 |
2.426 |
-0.401 |
z |
-0.615 |
-0.401 |
1.706 |
<r2> (average value of r
2) Å
2
<r2> |
90.616 |
(<r2>)1/2 |
9.519 |